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The Lorentz force
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Created on April 10, 2020
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Transcript
the lorentz force
How does a charge in motion feel the effect of a Magnetic Field in the surroundings?
The Lorentz Force
Vector Formula
Get a Uniform Magnetic Field
Scalar Formula
The Lorentz Force
The Lorentz Force
To find out the direction of the Lorentz force F you need to apply the Right-Hand-rule
The Right-Hand-Rule
Conventional symbols for vector B
B: OUT B: IN
Virtual lab: a charge in motion in a Magnetic field
The Lorentz Force is always perpendicular to both velocity (v) and displacement (s) of the charge
The work done upon q by the Lorentz Force to move it from A to B, is always zero!
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So, how does a charge in motion feel the effect of a Magnetic Field in the surroundings?
When a charged particle moves through a magnetic field, it experiences a Lorentz Force, providing it is not moving parallel to the field. This force acts at right angles to both the velocity of the particle, v, and the magnetic field, B.
The direction of this force depends on the direction of the velocity of the particle and the magnetic field as well as the sign of the charge of the particle.
From left to right: four examples of the Lorentz force, a simulation, a video about a moving charge in a uniform B.
v not parallel to B
v parallel to B
v perpendicular to B
α= 0°, sin0°=0 Uniform Motion of q
α= 90°, sin90°=1 Uniform Circular Motion of q
0°<α<90° Helical Motion of q (UM +UCM)
The motion of a charge under the effect of a uniform Magnetic Field B, as the angle between v and B changes .
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F=qvB is at right angle with v, then it is a centripetal force: q moves in a Uniform Circular Motion
v perpendicular to B
Flux and Circulation of the Magnetic Field
The previous are two quantities that can be defined for all vector fields, and are useful to describe some important properties of them.
Flux of the Magnetic Field
Given a uniform magnetic field B and a plane surface S, the magnetic field flux through S is given by:
Flux of the Magnetic Field
Gauss Law for Magnetic Fields
Gauss’s law for magnetism states that the total flux through a closed surface must be zero, and this implies that no magnetic monopoles exists
The number of magnetic field-lines which enter a closed surface is always equal to the number of field-lines which leave the surface. In other words: Magnetic field-lines form closed loops which never begin or end.
Gauss Law for Electric Fields
The electric flux through any closed surface is directly proportional to the net electric charge enclosed by that surface.
Thus, magnetic field-lines behave in a quite different manner to electric field-lines, which begin on positive charges, end on negative charges.Hence, a positive (negative) charge inside a closed surface generate an Electric field whose flux is positive (negative).
Circulation of the Magnetic Field
We calculate circulation of magnetic field B around a closed path by summing the dot product B ⋅ Δ l for every piece Δ l , treated as vector whose direction is the direction of traversal, and sum them all.
Circulation of B: Ampere Law
Ampere Law
Circulation of B: Ampere Law
Ampere Law
Ampere's Law states that for any closed loop path, the sum of the length elements times the magnetic field in the direction of the length element (the Circulation of B) is equal to the permeability times the electric current enclosed in the loop.